예술
뷰티 및 웰니스
공예
문화 및 역사
엔터테인먼트
환경
음식 및 음료
역공학
과학
스포츠
기술
웨어러블
The Semiconductor Laser Diode
Ed

작성자

Ed

30. 8월 2026FI
15
0
0
0
0

The Semiconductor Laser Diode

In the autumn of 1962 four groups reported a laser made from a piece of gallium arsenide the size of a grain of salt: Robert Hall at General Electric Schenectady, Marshall Nathan at IBM, Nick Holonyak at GE Syracuse with the first visible one, and Quist and Rediker at MIT Lincoln Laboratory. All of them worked only in pulses, and only when dunked in liquid nitrogen. The reason is that a plain GaAs junction confines nothing. Injected carriers wander off before they recombine, and the light spreads out of the thin active region into absorbing material. The threshold current density was tens of thousands of amps per square centimetre, which a chip can only survive for a microsecond at a time. The fix took eight years and arrived twice at once in 1970: Zhores Alferov's group at the Ioffe Institute and Izuo Hayashi and Morton Panish at Bell Labs both made the DOUBLE HETEROSTRUCTURE work. Sandwich a thin layer of GaAs between two layers of AlGaAs, which has a wider bandgap AND a lower refractive index, and you get both confinements from one sandwich: the carriers cannot climb out, and the light is trapped in a waveguide. Threshold fell by a factor of about a hundred and the diode ran continuously at room temperature. Alferov and Herbert Kroemer shared the 2000 Nobel Prize for it. FULLY BUILDABLE. This blueprint is the sibling of the LED blueprint, and the difference between them is measurable in an afternoon: build a proper current-source driver, sweep the current, and find the knee where the same junction stops being an LED and starts being a laser. The driver is the real skill here, because the commonest way a maker destroys a laser diode is by driving it from a voltage source.
중급
5 hours

안내

1

Start from the LED

Build or re-read the LED blueprint first. A laser diode is the same forward-biased junction, injecting electrons and holes into the same active layer, recombining across the same bandgap. Everything about the colour is identical. Two things are added, and only two. A CAVITY: the crystal is cleaved along a lattice plane, and the refractive index step from about 3.5 to 1.0 at the cleaved face reflects roughly 30 % without any coating at all. Two parallel cleaved faces are a Fabry-Perot cavity that costs nothing to make. And ENOUGH CURRENT to invert the junction, so stimulated emission outruns spontaneous. Keep the LED on the bench. You will sweep both and compare the curves.

필요한 도구:

Breadboard - ClassicBreadboard - Classic
점퍼 와이어 세트점퍼 와이어 세트
저항 키트저항 키트
실험실급 디지털 멀티미터실험실급 디지털 멀티미터
2

Build the constant-current driver

Build the driver on the breadboard. The op-amp holds the voltage across R_SENSE equal to the command voltage, so the diode current is V_SET divided by 10 ohms and nothing the diode does can change it. Use an LM358, not a TL071: on a single 5 V supply the LM358's inputs work down to 0 V, and this circuit commands 0 to 0.59 V. R1 (75k) over the 10k pot caps the command at 0.59 V, about 58 mA. Three details are not optional. R_SS and C_SS ramp the command with a time constant of about a second, because a laser diode is killed by a switch-on SPIKE far more often than by a steady overcurrent. D_PROT clamps reverse voltage, because the reverse breakdown of a laser diode is only a few volts. C_COMP with R_F damps the loop so a change of setting does not overshoot into the diode. Checked in ngspice: the current follows V_SET / 10 ohms to within 0.4 % (the transistor's base current) from 0 to 60 mA; switched on at full setting it rises smoothly to 58 mA, 63 % at 1.1 s and 99 % at 5.5 s, with no spike; a 10 mA step overshoots by about 0.9 mA without C_COMP and not at all with it. The simulation used a behavioural LM358-class op-amp and generic transistor and diode models, not vendor models, so it proves the circuit's behaviour, not your parts' exact figures. Before connecting the diode, test the loop with an ordinary red LED in its place and verify with the multimeter that the current follows the pot and holds steady when you warm the LED with your fingers.

KiCanvas 뷰어 로딩 중...

전문 PCB 디자인 뷰어

이 단계의 재료:

연산 증폭기 IC연산 증폭기 IC1 개
NPN 트랜지스터NPN 트랜지스터1 개
차단 다이오드(쇼트키)차단 다이오드(쇼트키)1 개
LED 키트LED 키트1 개
연산 증폭기 IC연산 증폭기 IC1 개
NPN 트랜지스터NPN 트랜지스터1 개
차단 다이오드(쇼트키)차단 다이오드(쇼트키)1 개
LED 키트LED 키트1 개
저항 키트저항 키트1 개
커패시터 키트커패시터 키트1 개
10 킬로옴 직선형 포텐쇼미터10 킬로옴 직선형 포텐쇼미터1 개

필요한 도구:

Breadboard - ClassicBreadboard - Classic
점퍼 와이어 세트점퍼 와이어 세트
실험실급 디지털 멀티미터실험실급 디지털 멀티미터
직류 전원 공급기직류 전원 공급기
3

Sweep the current and log the light

Wire GPIO25 to the driver's command input in place of the pot wiper, and the monitor photodiode through R_MON to GPIO34. Set I_MAX_MA below your diode's absolute maximum from its datasheet before you flash anything. Wear the goggles and point the diode into a matte card. Open the serial monitor at 115200 and capture the CSV. The sketch starts dark, measures the dark level, steps up in forty points with a 5 s settle at each, about three and a half minutes in all, and finishes dark. The settle matters twice: the slow-start filter needs five time constants to reach each new setting (at 40 ms the current has moved only a few percent of the way), and read too fast you would also catch the junction warming up rather than the L-I curve. The sketch reports the current the DAC actually commands, in steps of about 1.3 mA, not the value it asked for.
laser_diode_li_sweep.inocpp
// L-I sweep for a laser diode: ESP32 ramps the driver's command voltage and reads the
// monitor photodiode, printing CSV you can paste straight into the notebook.
//
// SAFETY. Wear the goggles. Point the diode into a beam dump or a matte card, never at a
// wall you might glance along. Never run the sweep with the diode uncollimated and facing
// up. Check the diode's absolute maximum current on its datasheet and set I_MAX_MA BELOW
// it -- a laser diode has no thermal margin worth speaking of and dies in microseconds.
//
// Wiring:
//   GPIO25 (DAC1) -> driver command input (replaces RV1's wiper)
//   GPIO34 (ADC1) -> monitor photodiode across R_MON
//   ESP32 GND     -> driver GND, one point only

const int PIN_CMD = 25;      // DAC output, 8 bit, 0..3.3 V
const int PIN_MON = 34;      // ADC1, safe to use while WiFi is active

const float R_SENSE   = 10.0;   // ohm, must match the driver
const float I_MAX_MA  = 60.0;   // <-- SET FROM YOUR DIODE'S DATASHEET
const int   N_POINTS  = 40;
const int   N_AVG     = 64;     // ADC averages per point
const int   SETTLE_MS = 5000;   // five time constants of the driver's 1 s slow start (R_SS 100k, C_SS 10u)

float readMonitor() {
  long acc = 0;
  for (int i = 0; i < N_AVG; i++) { acc += analogRead(PIN_MON); delayMicroseconds(200); }
  return (float)acc / N_AVG;
}

void setup() {
  Serial.begin(115200);
  delay(300);
  analogReadResolution(12);
  analogSetPinAttenuation(PIN_MON, ADC_11db);

  dacWrite(PIN_CMD, 0);          // start dark, always
  delay(500);
  float dark = readMonitor();

  Serial.println("# L-I sweep");
  Serial.printf("# R_SENSE = %.1f ohm, dark level = %.1f counts\n", R_SENSE, dark);
  Serial.println("current_mA,monitor_counts,monitor_minus_dark");

  // V_cmd = I * R_SENSE. The DAC is 8 bit over 0..3.3 V.
  float v_max = (I_MAX_MA / 1000.0) * R_SENSE;
  for (int k = 0; k <= N_POINTS; k++) {
    float v_cmd = v_max * k / N_POINTS;
    int   dac   = (int)(v_cmd / 3.3 * 255.0 + 0.5);
    if (dac > 255) dac = 255;
    dacWrite(PIN_CMD, dac);
    delay(SETTLE_MS);
    float m = readMonitor();
    float v_dac = dac * 3.3 / 255.0;                 // what the 8-bit DAC really sets: ~12.9 mV per count
    float i_mA = (v_dac / R_SENSE) * 1000.0;         // so the current moves in ~1.3 mA steps
    Serial.printf("%.2f,%.1f,%.1f\n", i_mA, m, m - dark);
  }

  dacWrite(PIN_CMD, 0);          // and finish dark
  Serial.println("# done, diode off");
}

void loop() {}

이 단계의 재료:

레이저 다이오드레이저 다이오드1 개
포토다이오드(BPW34)포토다이오드(BPW34)1 개
저항 키트저항 키트1 개

필요한 도구:

ESP32 개발 보드ESP32 개발 보드
Breadboard - ClassicBreadboard - Classic
점퍼 와이어 세트점퍼 와이어 세트
레이저 보안경레이저 보안경
데스크톱 컴퓨터데스크톱 컴퓨터
실험실급 디지털 멀티미터실험실급 디지털 멀티미터
4

Find the knee, the slope and the temperature coefficient

Jupyter 노트북 불러오는 중…

필요한 도구:

데스크톱 컴퓨터데스크톱 컴퓨터
5

Compendium: from liquid nitrogen to the fibre link

WHY 1962 NEEDED LIQUID NITROGEN. A homojunction confines neither carriers nor light. Injected electrons diffuse a micrometre or more before recombining and the optical mode spills into absorbing material either side, so threshold current density ran to tens of thousands of amps per square centimetre at room temperature — survivable only in microsecond pulses at 77 K. WHAT THE DOUBLE HETEROSTRUCTURE CHANGED. AlGaAs has both a wider bandgap and a lower refractive index than GaAs, so a thin GaAs layer between two AlGaAs layers is simultaneously a potential well for carriers and a dielectric waveguide for photons. Both confinements from one sandwich, and threshold current density fell to the low hundreds of amps per square centimetre. Alferov at the Ioffe Institute, and Hayashi and Panish at Bell Labs, reached room-temperature continuous operation independently in 1970. THE FACETS ARE THE CAVITY. The chip is cleaved along a crystal plane, giving two mirrors flat to atomic dimensions and parallel by construction, with about 30 % reflectivity uncoated from the index step of 3.5 to 1.0. Put L = 300 micrometres into the Fabry-Perot blueprint's free spectral range and the modes come out about 140 GHz apart — which is why a bare Fabry-Perot diode emits a comb of lines rather than one, and why telecom lasers add a distributed Bragg grating to pick a single mode. SIBLING TABLE AGAINST THE LED. LED: no cavity, spontaneous emission only, 20 to 40 nm wide, Lambertian, no threshold, tolerant of any old supply and a series resistor. Laser diode: cleaved-facet cavity, stimulated emission above threshold, about 1 nm wide, a beam roughly 10 by 30 degrees, a sharp threshold, and an absolute requirement for a current source. Below threshold the laser diode IS an LED, and you measured the changeover in step 4. WHERE THIS LEADS. The laser-communicator blueprint in the catalogue modulates a laser module with audio; that module is this blueprint's subject. Everything after this in the batch assumes a source like it — small, cheap, directly modulated at gigahertz rates by varying its current, and working at 1310 or 1550 nm instead of red.

재료

9

필요 도구

8

CC0 퍼블릭 도메인

이 블루프린트는 CC0로 공개되었습니다. 어떤 목적으로든 자유롭게 복사, 수정, 배포 및 사용할 수 있습니다.

제품 구매를 통해 메이커를 지원하세요. 판매자가 설정한 메이커 커미션 을 받거나, 이 블루프린트의 새로운 반복을 만들어 연결로 포함시킬 수 있습니다.

토론

(0)

로그인 하여 토론에 참여하세요

댓글 로딩 중...